An additional explanation of the two attractors has to be made. The \(\lbrace 0,1,1\rbrace \)  attractor has been well-discussed in literature [1]}, [2]}, [3]}. With this attractor, the BH tightly follows the \(\lbrace 0,1,1\rbrace \)  Regge trajectory, determined by \(J=a_{*C}^{011} M^2\)  in the mass-spin plot. To the contrary, the \(\lbrace 1,1,1\rbrace \)  attractor is approximately given by,
\(M_s^{(011)} \omega _I^{(011)} + M_s^{(111)} \omega _I^{(111)} = 0.\) 
